Home > Research > Publications & Outputs > Tuning the thermoelectric properties of metallo...

Electronic data

  • c5nr06966a

    Final published version, 1.49 MB, PDF document

    Available under license: CC BY: Creative Commons Attribution 4.0 International License

Links

Text available via DOI:

View graph of relations

Tuning the thermoelectric properties of metallo-porphyrins

Research output: Contribution to Journal/MagazineJournal articlepeer-review

Published

Standard

Tuning the thermoelectric properties of metallo-porphyrins. / Al-Galiby, Qusiy; Sadeghi, Hatef; Algharagholy, Laith et al.
In: Nanoscale, Vol. 2016, No. 4, 28.01.2016, p. 2428-2433.

Research output: Contribution to Journal/MagazineJournal articlepeer-review

Harvard

APA

Vancouver

Al-Galiby Q, Sadeghi H, Algharagholy L, Grace IM, Lambert CJ. Tuning the thermoelectric properties of metallo-porphyrins. Nanoscale. 2016 Jan 28;2016(4):2428-2433. Epub 2016 Jan 5. doi: 10.1039/C5NR06966A

Author

Al-Galiby, Qusiy ; Sadeghi, Hatef ; Algharagholy, Laith et al. / Tuning the thermoelectric properties of metallo-porphyrins. In: Nanoscale. 2016 ; Vol. 2016, No. 4. pp. 2428-2433.

Bibtex

@article{b077882efe814295984abcc1ff25402a,
title = "Tuning the thermoelectric properties of metallo-porphyrins",
abstract = "We investigated the thermoelectric properties of metalloporphyrins connected by thiol anchor groups to gold electrodes. By varying the transition metal-centre over the family Mn, Co, Ni, Cu, Fe, and Zn we are able to tune the molecular energy levels relative to the Fermi energy of the electrodes. The resulting single-molecule room-temperature thermopowers range from almost zero for Co and Cu centres, to +80 μV K−1 and +230 μV K−1 for Ni and Zn respectively. In contrast, the thermopowers with Mn(II) or Fe(II) metal centres are negative and lie in the range −280 to −260 μV K−1. Complexing these with a counter anion to form Fe(III) and Mn(III) changes both the sign and magnitude of their thermopowers to +218 and +95 respectively. The room-temperature power factors of Mn(II), Mn(III), Fe(III), Zn and Fe(II) porphyrins are predicted to be 5.9 × 10−5 W m−1 K−2, 5.4 × 10−4 W m−1 K−2, 9.5 × 10−4 W m−1 K−2, 1.6 × 10−4 W m−1 K−2 and 2.3 × 10−4 W m−1 K−2 respectively, which makes these attractive materials for molecular-scale thermoelectric devices.",
author = "Qusiy Al-Galiby and Hatef Sadeghi and Laith Algharagholy and Grace, {Iain Mark} and Lambert, {Colin John}",
year = "2016",
month = jan,
day = "28",
doi = "10.1039/C5NR06966A",
language = "English",
volume = "2016",
pages = "2428--2433",
journal = "Nanoscale",
issn = "2040-3364",
publisher = "Royal Society of Chemistry",
number = "4",

}

RIS

TY - JOUR

T1 - Tuning the thermoelectric properties of metallo-porphyrins

AU - Al-Galiby, Qusiy

AU - Sadeghi, Hatef

AU - Algharagholy, Laith

AU - Grace, Iain Mark

AU - Lambert, Colin John

PY - 2016/1/28

Y1 - 2016/1/28

N2 - We investigated the thermoelectric properties of metalloporphyrins connected by thiol anchor groups to gold electrodes. By varying the transition metal-centre over the family Mn, Co, Ni, Cu, Fe, and Zn we are able to tune the molecular energy levels relative to the Fermi energy of the electrodes. The resulting single-molecule room-temperature thermopowers range from almost zero for Co and Cu centres, to +80 μV K−1 and +230 μV K−1 for Ni and Zn respectively. In contrast, the thermopowers with Mn(II) or Fe(II) metal centres are negative and lie in the range −280 to −260 μV K−1. Complexing these with a counter anion to form Fe(III) and Mn(III) changes both the sign and magnitude of their thermopowers to +218 and +95 respectively. The room-temperature power factors of Mn(II), Mn(III), Fe(III), Zn and Fe(II) porphyrins are predicted to be 5.9 × 10−5 W m−1 K−2, 5.4 × 10−4 W m−1 K−2, 9.5 × 10−4 W m−1 K−2, 1.6 × 10−4 W m−1 K−2 and 2.3 × 10−4 W m−1 K−2 respectively, which makes these attractive materials for molecular-scale thermoelectric devices.

AB - We investigated the thermoelectric properties of metalloporphyrins connected by thiol anchor groups to gold electrodes. By varying the transition metal-centre over the family Mn, Co, Ni, Cu, Fe, and Zn we are able to tune the molecular energy levels relative to the Fermi energy of the electrodes. The resulting single-molecule room-temperature thermopowers range from almost zero for Co and Cu centres, to +80 μV K−1 and +230 μV K−1 for Ni and Zn respectively. In contrast, the thermopowers with Mn(II) or Fe(II) metal centres are negative and lie in the range −280 to −260 μV K−1. Complexing these with a counter anion to form Fe(III) and Mn(III) changes both the sign and magnitude of their thermopowers to +218 and +95 respectively. The room-temperature power factors of Mn(II), Mn(III), Fe(III), Zn and Fe(II) porphyrins are predicted to be 5.9 × 10−5 W m−1 K−2, 5.4 × 10−4 W m−1 K−2, 9.5 × 10−4 W m−1 K−2, 1.6 × 10−4 W m−1 K−2 and 2.3 × 10−4 W m−1 K−2 respectively, which makes these attractive materials for molecular-scale thermoelectric devices.

U2 - 10.1039/C5NR06966A

DO - 10.1039/C5NR06966A

M3 - Journal article

VL - 2016

SP - 2428

EP - 2433

JO - Nanoscale

JF - Nanoscale

SN - 2040-3364

IS - 4

ER -